#groups-rings-fields
1 messages · Page 238 of 1
is your book looking at group actions from a categorical perspective or something
Mathematical crippling
It's explaining group theory with category theory
is this your introduction to group theory or are you doing this just for funsies - also what's the name of the book? I'm curious
fair enough
I read into some HoTT for fun before, but it's a little abstract without any other mathematical knowledge
Aluffi is a funny name
I did read about category theory before but that had mostly examples in Set... Well and Cat but well, without concrete examples it's not easy to understand. Some people said to look at Abstract Algebra first
I hope you get something out of it, but please don't write off the theory as a whole before you've seen the non-categorical intro!
Oh I think it's pretty fun. Already gave some more insights into CT and even HoTT
Well it's not just a categorical intro, it's from both views I think
Next page he describes it as an operation on sets, right?
BE NOT AFRAID ass shit
But is non standard a problem?
Since I read something about CT in think it is fun to explore both at the same time
I like aluffi
Instead of reading about AA and learning CT Awodey style...
That's the book I learned algebra from
Cool
he defines stuff using the most important definition (categories) so i like it
sotrue!
I have question is this enough
Let G act transtively on X, and let N be a normal subgroup of G. Prove that the orbits of X under N are all the same size; in other words: for all x and y in X, $#Nx$ = $#Ny$.
\begin{proof}
First of all, we know that N is a subgroup of G and it is normal, so this means for all $g\in G$ and $h \in N$ the following applies $ghg^{-1} \in N$. We know that $G$ is transitive, so this means that there is one orbit. Take two elements from $N_x$, for example $x$ and $x_1$, then the following applies
\begin{equation*}
h \circ x = x_1 \text{ for a $h \in N$ }
\end{equation*}
We also know that $G$ is transitive, so this means that
\begin{equation*}
g \circ x = y \text{ for a given $g \in G$}
\end{equation*}
We now know that the following must apply:
\begin{equation*}
x = g^{-1} y
\end{equation*}
We can now substitute this above and we get the following:
\begin{equation*}
h \circ g^{-1} y = x_1 \leftrightarrow h g^{-1} \circ y = x_1
\end{equation*}
It follows from this:
\begin{equation*}
g h g^{-1} \circ y = g\circ x_1
\end{equation*}
note that $ghg^{-1} \in N$ so this now means that:
\begin{equation*}
n\circ y = g\circ x_1
\end{equation*}
\end{proof}
Mootje
Looks good, but it would be more readable if you said a little bit more about what you're doing.
Like presumably you're saying that multiplication by g defines a bijection between Nx and Ny, so maybe at least say that
Then it can also be much shorter, like gNx = (gN)x = (Ng)x = N(gx) = Ny
But does this implies then they are equal in size
But does this implies then they are equal in size
That’s what I’m afraid about
If you have a bijection between two sets, they are equal in size yes.
Often that's actually the definition of two sets having the same size
i have this elementary question
let x, y be nonzero divisors of R. then (R/xR)/(yR/xR) is just R/(x, y)R, right?
Commutative ring?
this should be a statement about the fact that "quotients commute"
ya
but i don't see it exactly
That’s third iso I think
feel that? that's the third iso theorem
sure something like that
Sniped
i want the fancy way though
(x,y) = (x) + (y) no?
ya
what happens when you quotient out (x) or (y) then 
Doesn't third iso give us (R/xR)/(yR/xR) \cong R/yR though
It does ye
exactly by this logic
ok so you're not saying it is R/(x,y)R
what is this cursedness
xR is not contained in yR


wew edit that gif of the guy releasing the trunk monkeys to be sully emojis
anyway I realise that, if it was a quotient of rings, that this would just be yR because xR \subseteq yR
so it makes sense there
what's wrong with what i said
since R/xR is an R-module y gives an action on R/xR
and y(R/xR) is defined to be the image of that action
which is a submodule of R/xR
which we quotient by
it was absolutely not clear at all that this was a quotient of modules
you could've just been working with non-unital rings
which is what we both assumed was happening
wait... even for modules you can't quotient by something that isn't a submodule
is there a non submodule somewhere
sure thanks alot
I have one more question
im suppose to prove that a 4d dimensional cube has 192 symmetris
or with other words that he has 8 elemnts of orbit and 24 elements of stabilizator
is there an easy way to do that
192? that seems strange.
Well, the symmetry group of a tesseract act transitively on the faces, and there are 8 faces. Each face is a cube and they have 24 symmetries
jagr am I skill issuing here? It's definitely S_2 \wr S_4 right
So does that mean that if a cube has 24 symmetry then the 4d cube has also 24
jagr practically told you that it's 8*24, which is 192
24 permutations of each face, and then 8 faces for a total of 192
With reflections maybe?
yeah that's with reflections
ok if cubes have 24 symmetries we're definitely without reflections
mb
do you know that the group of rotations of a cube is S_4?
the canonical way to do that is to look at how the rotations act on the 4 main diagonals of the cube
but there might be an easier way
yeah there is, I think
If you just need that there's 24 of them, then you can repeat the argument I guess
yeah, but then do we need that there are four rotations of a square? 
I'm gonna exposit the way I just came up with because I think it's nice
nvm it's basically just the "permute the diagonals" argument in fancy clothes
hi guys sorry to interrupt, needed some help with a concept. Im doing quotient groups of rings and have always been given distinct equivalence classes for quotient groups by my professor. Im not sure how to get these, or how to tell how many equiv classes there should be for a given quotient group
any help would be super appreciated 😦
equivalence classes for quotient groups are exactly the cosets
you're quotienting by the relation g ~ g' iff gH = g'H, so the equivalence class of g is gH
this is the problem i dont really understand
for polynomial rings do i divide the polynomials and find the euiv classes that way?
who the hell is a .HEIC
😭
u running discord on a CDC 7600 or something
no, the equivalence classes are the sets a+(x^2+x+1)
you can't divide polynomials in Z_2[x], it isn't a field
ohhhhhh
thank u sooo much!!!!
Source
I'll do this REALLY explicitly if you want
the idea behind quotients is that you're "adding relations in" to your object
so by quotienting out by (x^2+x+1), you're essentially saying "give me Z_2[x], but set x^2+x+1 = 0"
which is why all of our equivalence classes are only linear polynomials! because as soon as you see an x^2 you can go "hmm... since x^2+x+1 = 0, x^2 = x+1 (remember we're in Z_2 here, so -x = x)" and replace x^2 with a linear polynomial
thank u so much ur a life saver
Finitely accessible
lol
"playing pretend"
good mo post
it's the correct way to think about quotients
they turn equivalence relations into actual equality
it is something one should be aware of, and of course one cannot proclaim one approach better another without knowing both
i’ve been reading coxeter and moser’s generators and relations and struggling with making sense of this 
esp with like making sense of what exactly is the relationship between the hyperbolic triangle reflection groups Δ(infty,infty,infty), Δ(2,3,infty) and SL(2,Z)
i just know the modular group is isomorphic to a index two subgroup of Δ(2,3,infty), namely the rotational or von Dyck triangle group D(2,3,infty)
which is wack
oh wait hold on
no I'm thinking of affine reflection groups
which is the most boring case of what you're talking about
well
I thought (2, 3 infty) is the modular group
it is
but index 2 here?
yes
😮
some people are not so explicit whether they are talking about the von Dyck or the full triangle group
oh maybe idk what triangle is vs von dyck
I'm always suspicious of SL(2,Z). It's an omen for weird things
that would probably be Δ(infty,infty,infty) which is the free group over three order two generators
ok, but the math doesn't change, right? 😛
free abelian surely?
ohh so von dyck subgroup is the orientation preserving stuff
no
or am I visualising this wrong
ahhhh no you're right, there's a "sign error". And by that I mean the orientation is different
dw i prolly am too
typically these are presented purely abstractly anyways
that's boring! I like picturing one of those scary fair ground mirror mazes
Δ(infty,infty,infty) would be like being stuck in a cube of mirrors... most terrifying indeed...
Δ(l,m,n) is < L, M, N | L^2 = M^2 = N^2 = (LM)^l = (MN)^m = (NL)^n = 1 >
oh they're just coexter groups
aye
duh. of course they are. They're reflection groups
and x^infty = 1 is vacous, so no relations on x
yur
so Δ(infty,infty,infty) is < L,M,N | L^2 = M^2 = N^2 = 1 >
Δ(3,3,3) is S_4 right?
IIRC this is PGL(2,Z)
this is jolly good fun...
No
WHAT
That’s Δ(2,3,3)
rats
that’s a euclidean reflection group… which i’ve honestly spent way too little time on
oh yeah duh. (12) and (34)
Δ(2,3,5) is also a nice one
I swear I read the wikipedia page about these like years ago
may be viz like the second of these: #math-discussion message
The finite triangle groups are precisely (2,2,n), (2,3,3), (2,3,4), and (2,3,5)
are these the ones for positive curvature space
well they'd have to be right?
Yes
or else you just keep going foreverrrr
they provide tesselations of the sphere ye
The are the symmetry groups of the dihedra and hosohedra, the tetrahedron, the cube and octahedron, and the dodecahedron and icosahedron, respectively
this thing has Δ(2,3,5) symmetry
I need to learn about these groups. This is so cool
This is wrong btw
something something central extenstion of PSL(2,Z)
something something C_3 \ast C_2
do you study combinatorics or something
oh absolutely not
shame, coexter groups are very nice combinatorially
(2,3,∞) is PGL(2,Z)
(∞,∞,∞) has the free group on two generators as an index-2 subgroup, but I don’t remember whether or not it’s the direct product
I wonder what happens if you... put more numbers in...
obviously it's n-dimensional space at that point but
Then you get Coxeter groups of higher rank
is there anything funny?
Yeah
please tell
You actually need (n²-n)/2 numbers to specify a Coxeter group of rank n
explains why 3 numbers give tilings of a 2-dimensional surface
wiat does it
hold the phone 📱
These numbers correspond to the angles between facets of the fundamental domain
I'm looking at the pictures on the wikipedia page, it seems like it determines how many triangles "touch" at a given corner
Yes
right now it makes sense I think
there's 3 corners on a triangle, so you need 3 numbers
and it has that particular presentation because the product of two reflections looks like a rotation around a corner (I think?)
so if after n reflections you end up back at the start, (xy)^n = 1
aye
i'm sure that exists already
I did
a (l,m,n) triangle group has as a fundamental domain a Schwarz triangle with angles pi/l,pi/m/pi/n
We can represent Coxeter groups as labeled graphs by assigning each generating reflection a vertex. Then, the edge between them tells you the order of their product: if it’s 2, there is edge, if it’s 3, there is an unlabeled edge, and if it’s more than 3, there is an edge which is labeled with that value.
These are called Coxeter-Dynkin diagrams
I know about them cause of rep theory
i see them all over the place but haven't bothered trying to make sense of them
thinking about the generalisation here, if we just look at the simplicial complex consisting of an n-simplex but with the actual n-simplex removed, then you have (n+1) reflections as previously stated, and then the order of the product in the corrisponding Weyl group is the number of ``hollow" simplices around each 1-simplex I think? The trick is then trying to move this to general complexes
at least I have very good motivation to care about tits buildings now
are you familiar with the geometry side of things?
Here’s something cursed you can do: if you interpret the edge labels as just the fraction of pi that the angle forms, there’s nothing stopping you from using fractional labels.
actually those appeared when i was trying to make sense of the relation between (2,3,infty) and (infty,infty,infty) and i noped out
These don’t correspond nicely to presentations, though.
irrational labels 
or wait would they just be (\infty, \infty, \infty)
one thing i noticed is that a (infty,infty,infty) triangle can be formed by gluing together six (2,3,infty) triangles but i'm not sure how that correspond to the algebra side of things
there is a really nice thing here actually
that's a good observation
algebraic "gluing" is a quotient (more generally, a colimit)
Here are the 5 Coxeter-Dynkin diagrams that generate tetrahedral symmetry
this is SO cursed
That means (∞,∞,∞) is an index-6 subgroup of (2,3 ∞)
that is what i was suspecting but i'm not sure how to show it formally 😭
^
teehee
if ur a geometer u can just say "glue" and it'll be fine
cause that's all u mfs do anyway
ok i'll do just that, thanku for the pro tip
though i desperately need to actually learn elementary group theory
You can also label the vertices of Coxeter-Dynkin diagrams to represent uniform polytopes.
no time atm though, bachelor thesis due in 4 days and i've only written like 20% of what i intend (after cutting down on what i wanted to include drastically)
since you're working with presentations I'll give you this tip: if you have a presentation <X|R> of a group G and <X|S> is a presentation of a normal subgroup in the same generator set, then G/N = <X|R union S>
uwu
alternatively, if you want to add a set of relators S, you take the normal closure of S and then take the quotient
thanku thanku very much
this is how everyone should think about quotients
I don’t entirely remember how this works, though
also this article is amazing (though i've only taken the time to understand the first half)
No it isn’t
it looks EXACLTY like E_8
It’s H_4
union of the orbits of the elements I'd guess
Wythoff Construction
I see
Can we use the orbit stabilizer theroem
Orem
If the stabiliser is a set
Not an element
if your group is acting on X but you care about orbits on subsets of X, you can extend the action to a group action on the power set of X
then use orbit stabiliser there
group actions are very general, but while this indeed is possible, i suspect you're overcomplicating things here Mootje
though actually sometimes "overcomplicating" things yields lovely new insights mwahaha
Thanks
Idk if someone wants to check my prove
Cause I’m using matrices
@hidden wind
hi
it may even be a subgroup
And elements are usually sets anyway
this is what
i did
\begin{equation*}
G := {g \in SO(4)|g(H) = H}
\end{equation*}
prove that $# G = 192$
\begin{proof}
First I'm going to find the number of elements of the stabilizer in $K_1$ since that's easier and then I'm going to prove that the action is transitive. To find the number of elements of stabilizer we have to follow the following steps. We know that $K_1$ has the following form:
\begin{equation*}
K_1 = {(x,y,z,w) \in H | x = 1}
\end{equation*}
This means that an element from $K_1$ must have the following form: $(1,y,z,w)$. However, we should note that the orthogonal group of $SO(4)$ is defined as follows:
\begin{equation*}
SO(4) = {g\in GL_4(\mathbb{R}) \mid g^{t}g = 1, det(g) = 1}
\end{equation*}
We further know that $SO(4)$ can be seen as the rotation around the origin of our four-dimensional cube. Since that element $x$ must be equal to one, the matrix rotation must look like this:
\begin{equation*}
\begin{pmatrix}
1 & W \
W^T & A
\end{pmatrix}
\end{equation*}
The above matrix is a $4 \times 4$ matrices. Where $W, W^t \in R^3$ and note that $A$ is a matrix of the form $A_{3\times 3}$. We further know that $g^tg$ must be equal to the identity and so this means that $WW^T = 0 $ This is of course only possible if $W = 0$ and therefore also $W = 0$. This means that there remains only matrix $A$ and this is a $3 \times 3$ matrix. so then for the rotation for the three dimensional cube we get the following matrix:
\begin{equation*}
\begin{pmatrix}
1 & 0 & 0 & 0 \
0 & \
0 & & SO(3)\
0 &
\end{pmatrix}
\end{equation*}
From here we just need to find the symmetry of $SO(3)$ and we know that they are equal to 24 so this means that the stabilizers of our $K_1$ is equal to 24.
\end{proof}
Mootje
im not really sure if that is good way
and the reason that i did that is the following
give me asecond
i send it
Let $H \subset \mathbb{R}^4$ be the 4-dimensional cube given by
${(x, y, z, w) \in \mathbb{R}^4 \mid -1 \leq x, y, z, w \leq 1}$
(so the four coordinates lie between $-1$ and $1$).
We define
$\text{SO}(4) = {g \in \text{GL}_4(\mathbb{R}) \mid g^tg = 1, \det(g) = 1}$.
The group $\text{SO}(4)$ can be understood as rotations around the origin of 4-dimensional Euclidean space. Each such rotation is given by choosing two planes $V, W \subset \mathbb{R}^4$ and two angles $\theta, \psi$, where the planes are perpendicular to each other, and then rotating by an angle $\theta$ in $V$, and an angle $\psi$ in $W$. For example,
[
\begin{pmatrix}
\cos(\theta) & -\sin(\theta) & 0 & 0 \
\sin(\theta) & \cos(\theta) & 0 & 0 \
0 & 0 & \cos(\psi) & -\sin(\psi) \
0 & 0 & \sin(\psi) & \cos(\psi)
\end{pmatrix}
]
is such a rotation, where we rotate by an angle $\theta$ in the $x, y$-plane, and by an angle $\psi$ in the $z, w$-plane.
The rotation group of $H$ is given by
$G := {g \in \text{SO}(4) \mid g(H) = H}$
as a subgroup of $\text{SO}(4)$.
Problem: Prove that $#G = 192$.
Hint: The group $G$ acts on the "sides" of $H$. These sides are themselves 3-dimensional cubes, given by
\begin{align*}
K1 &= {(x, y, z, w) \in H \mid x = 1} \
K2 &= {(x, y, z, w) \in H \mid y = 1} \
K3 &= {(x, y, z, w) \in H \mid z = 1} \
K4 &= {(x, y, z, w) \in H \mid w = 1} \
K5 &= {(x, y, z, w) \in H \mid x = -1} \
K6 &= {(x, y, z, w) \in H \mid y = -1} \
K7 &= {(x, y, z, w) \in H \mid z = -1} \
K8 &= {(x, y, z, w) \in H \mid w = -1}
\end{align*}
Prove that this action is transitive, determine the stabilizer of $K1$, and conclude using a theorem we have seen in class.
Mootje
this was the question
The only rotations that can map a plane to itself is quarter revolution rotations. Each plane has 3 faces / pair of orthogonal planes to it
what do you mean
i do not get it
I am sorta talking to myself, sorry
Let me check
Idk seems fine. I don’t know the required level of rigor for your class
My psycho way of doing things is to let it act on {0,1}^4
the thing is im not really sure if W W^t
are in a good place
and the second thing that im not sure about if WW^t = 0 then W and W ^T must be 0
Sounds right
MM^T must be 0 as a whole matrix
Consider the image of (1,0,0,0) must be fixed
Or at least to one of the other verticies
And the transpose from there
I shouldn’t be using discord at a red light brb
Oh wait. This is just the standard rep of S_4
so actually i should have written from her that in place of W^t mayb (1,0,0,0)
(1,0,0,0) must be mapped to one of the verticies of the cube where x = 1
sure but i do not really get what you want to say here
i mean sure the thing that we only know is that the following must be true
\begin(pmatrix)
1 & W \
0 & A \
0 & \
0 & \
\end{pmatrix}
this is what you mean
maybe
and what do you thing @delicate orchid
honestly, mootje? I like your proof. It's a good approach
it's just very explicit
thanks but is it good
is it a good approach
and now im struggling with now proving transitivity
or do you have some changes
I just... I just don't believe it's 192 though? I just don't
The hyperoctahedral group for $n=4$ is $S_4 \wr C_2$ which has order $24^2 \times 2$ which is like, 1152
Wew Lads Tbh
sure, the fact that they're special orthongal gets rid of that factor of 2, but it's still 24^2
hahaahah
I just don't even know what action is on the hyper cube here?
well i mena i just proved that the element in stabilisator are 24
are we allowed to pick up and rotate individual cubes?
and you have agreed with my prove
I agree with the approach
but well i still did not find the orbit to be equal to 8
thus
so we do not know if its correct
i just found that the stab equal to 24
because the size of this group just for the cube is absolutely massive
well no we're not allowed to do that because we're in SO(4) so we can only rotate
true
Isn’t it though?
how?
I think this proof works
every possible thing I've come up with is massive
I never doubted that
I just don't believe it
Probably you have written down things that are not rigid symmetries of the hypercube which preserve orientation
I haven't written anything down this is pure visualisation
Hmm well I think for visual proofs this approach is pretty good
Clearly the symmetries act transitively on the faces
yeah which is why I like it. Work with the rotations directly
well is my proof correct btw
So then we just have to compute the stabilizer of one face which is a vanilla flavored cube
or do you find it rigorous
and then that can be calculated to be S_4
can you post it? I have not read it
sure give me a second
SO(4) acts on verticies of the hypercube transitively, which corresponds to {0,1}^4. The orbit is therefore 2^4 = 16. Now it’s asking how many rotation stabilize a vertex, so for example consider the vertex (1,0,0,0). The vertex must be fixed here, so the matrix in SO(4) must have its first row and column be (1,0,0,0). Thus the remaining bit is the lower 3x3 matrix?
i will post new version
Of which must permute the remaining verticies?
\begin{equation*}
G := {g \in SO(4)|g(H) = H}
\end{equation*}
prove that $# G = 192$
\begin{proof}
First I'm going to find the number of elements of the stabilizer in $K_1$ since that's easier and then I'm going to prove that the action is transitive. To find the number of elements of stabilizer we have to follow the following steps. We know that $K_1$ has the following form:
\begin{equation*}
K_1 = {(x,y,z,w) \in H | x = 1}
\end{equation*}
This means that an element from $K_1$ must have the following form: $(1,y,z,w)$. However, we should note that the orthogonal group of $SO(4)$ is defined as follows:
\begin{equation*}
SO(4) = {g\in GL_4(\mathbb{R}) \mid g^{t}g = 1, det(g) = 1}
\end{equation*}
We further know that $SO(4)$ can be seen as the rotation around the origin of our four-dimensional cube. Since that element $x$ must be equal to one, the matrix rotation must look like this:
\begin{equation*}
\begin{pmatrix}
1 & W \
W^T & A
\end{pmatrix}
\end{equation*}
The above matrix is a $4 \times 4$ matrices. Where $W, W^t \in R^3$ and note that $A$ is a matrix of the form $A_{3\times 3}$. We further know that $g^tg$ must be equal to the identity and so this means that $WW^T = 0 $ This is of course only possible if $W = 0$ and therefore also $W = 0$. This means that there remains only matrix $A$ and this is a $3 \times 3$ matrix. so then for the rotation for the three dimensional cube we get the following matrix:
\begin{equation*}
\begin{pmatrix}
1 & 0 & 0 & 0 \
0 & \
0 & & SO(3)\
0 &
\end{pmatrix}
\end{equation*}
The reason that it must be a $SO(3)$ is very simple because we know one more thing that the determinant of the matrix must be equal to $1$ so this can either be the entire diagonal equal to $1$ or with the development of the minors we need to get determinant $1$ \end{proof}
Mootje
oh sorry
no
well im going to delete it
it's ok it's just very long
oh sure
yes but this my proof
i did not yet prove teransitivity
and idk how
but i found stabilsator is easier
transitivity is pretty clear
well i mean if its clear
than we get the orbit
but idk how the orbit must be 8 thought
to move one face to an opposite face, pick any other face's midpoint as your axis and rotate by 180 through it, for adjacent faces do the same thing but at a corner by uhh probably 90?
In a hypercube, shouldn't the vertices be (±1,¯1,±1,±1)? Things like (1,0,0,0) would be the vertices of, um, a hyper-ocathedron instead.
wait is the cube centred at the origin?
I did not understand this proof
u know what. It better be
yes
good
well you need to read the question
I assumed so, since the natural action of SO(4) fixes the origin.
i will tag the question
I know the question
true!
this
I don’t understand how you show that the upper left hand entry of the matrix is 1
read this
Should be 2^4 * 4! I think. So if you only consider rotations not reflections that's 2^3 * 4! = 192
In mathematics, a hyperoctahedral group is an important type of group that can be realized as the group of symmetries of a hypercube or of a cross-polytope. It was named by Alfred Young in 1930. Groups of this type are identified by a parameter n, the dimension of the hypercube.
As a Coxeter group it is of type Bn = Cn, and as a Weyl group it is...
that is far too much text for a problem I completely know about
am I just stupid. Oml did I get the wreath product backwards
hahahah i know
I got the wreath product backwards chat
but @delicate orchid how would you prove that its transitive
or the orb is equal to 8
I just said
oh wait what about the secret third kind of face
yes but this more of an intuition
Guess you can just explicitly argue that things like
(x, y, z, w) -> (z, x, y, w) and so on are symmetries
you have to be careful with orientation preserving
that is true
Ought just to be the even permutations then, right?
Then you have A4.
but A_4 acting transitively is... obvious?
yeah
we're fine
still cannot believe I remember the wreath product wrong
well the element of A4 are 12
one of my worst blunders
yeah, and we're acting on the basis vectors
So brain missed the centered at the origin part
except if the 24 that i found is wrong
A face is just what you get if you fix one cordinate, so this together with flipping two signs shows you you can move from any face to any other
no it isn't, we're saying that even permutations of the coordinate axes are in SO(4), and fix the cube
12×16 is 192, though, and the hypercube has 16 pairs of opposite vertices to preserve.
and this action is transitive
however its suppose to be 24
im sure about that
since you also agreed to my prove
and sure that the order must be 8\
Why not just look at the action on vectors of length one with only one nonzero entry
what? I never said it wasn't?!?!
well you said it is not
(can someone state in a single line what it is we're counting?)
Then you have the elements of SO(4) of the form diag(-1,-1, 1, 1) and all of the even permutations, and the group they generate
we're showing that the action is transitive I couldn't care less about the size of the stabiliser
and where?
This acts transitively
Rotational symmetries of tesseract
do not worry i read it wrong
You meant diag(-1,-1,1,1), I hope?
Yes
sure
Okay so that shows the action is transitive
Now the stabilizers of a face leave the midpoint of the face fixed
So wolog (1, 0, 0, 0) is fixed
Do we already have a known solid argument for 192, and we're looking for alternative ways to get the same?
so the matrix is block upper triangular and orthogonal, so it is a block matrix of the form you say
this is what we are suppose to prove
Yes
its true
Or rather
That was ... somewhat conflicting replies.
its given
wait really?
We have a sketch and are helping mootje fill in the details
oh ok!
The sketch is to look at the stabilizer of a face and use orbit stabilizer
but i assume that the amount of elements here must equal to 8
(My first reaction would be to say, we can permute the axes in 4! ways and for each of them choose signs in the permutation matrix in 2^4 ways, but half of those have the wrong determinant, so 4!·2^4/2 = 192).
i might be wrong though
I'm writing up a full proof of this as we speak
There are big stabilizers
and is what I had in my mind and would've said if I had not gotten the wreath product backwards!
But it doesn’t matter because we can compute the stabilizers later
sure
actually it doesn't matter tropo said it better than me lol
the orbit should be 8
well sorry
now im just sharing information
well the thing i do not get how to prove that
i mean sure we prove transitivity
and we know that transititvity implies
that there exist one orbit
but the thing is we have also find a stabilsator of a subset
not the whole set
here's what I had anyway:
Consider the set of reflections r_i sending e_i -> -e_i in R^4 and the group they generate. This group acts transitively on the faces of the hypercube. These have determinant -1 as linear transformations and are in O(4). The product of two reflections r_ir_j has determinant (-1)^2 = 1, and is thus in SO(4). Furthermore this product is a rotation, shown by an elementary examination of whatever dihedral group r_i, r_j generate in the plane <e_i, e_j>. These account for all rotations of the hypercube because \todo{explain why}
That’s why we’re helping
sure i appreciate as well
I don't mean to be rude but are you serious?
but i mean like if we prove that transitive then we must at the same time know the orbit
hahahah
well just forget about it
i mean i got confused
to be fair
To say "the action is transitive" nothing more or less than a fancy word for "there is a single orbit containing all the things".
i agree with that
and i was mentioning that like 10000 times
the thing that went wrong a lot is speaking that i missed the part
that we are suppose to prove
cuz im writing in latex in overleaf and coming back
so i got confused
and then Wew lads got angry
on me
I'm not really angry
sorry
it's alright but in future just make it clear when a problem has actually been solved so someone else doesn't get trolled online
sure
ok but now I am actually curious what this other problem is
So I’ve been thinking about elliptic curve cryptography recently and the possibility of incorporating it into my abstract algebra class. I’m wondering — do people use them much over finite fields of prime-power order rather than just prime order?
I’m looking to use applications to anchor why we study some of the things we do, so for example I’m going to be using the Rubik’s cube as an anchor for group theory.. I figured elliptic curve cryptography could be good for finite fields and other topics, especially if they can be analyzed over extension fields.
yeah there are some examples like this. For example people will often work in characteristic 2 in order to exploit binary representations of elements, and then the relevant curves are defined over finite fields F_{2^n}.
There are other examples like the FourQ curve which is defined over F_{p^2} for the Mersenne prime p=2^{127}-1
what about the fargues fontaine curve
Doesn’t some weird stuff happen when you’re in characteristic 2 though?
the weierstrass normal form won't work, you'll have to use a slightly different form of that. Probably other problems too lol
appears discord is using an elliptic curve digital signature algorithm currently, could look into this one specifically if you want feet-on-the-floor motivation:
the specific finite field features may be a small bit complicated if you’re against people just starting algebra and wont be specifically focused on the finite field stuff, still it is doable. I suggest you to check about error correcting codes, its a good bunch of linear algebra over finite fields and it uses in an essential way the basic knowledge of finite fields. Another suggestion is LFSR’s which are pseudo random generators which again to prove the main prosperties use the basic finite field properties in an essential way
both these thing are much more elementary than elliptic curves (still very very interesting and used in practice)
my supervisor telling me to keep on neglecting abstract algebra like a chad 
can someone verify this for me
pika
I'll look into those — could be very useful, thank you!
AES?
yeah
What's AES :V
advanced encryption standard, an encryption algorithm
Oh interesting
yeah it's pretty much used in most wireless security things
like WPA2 ( the thing ur using for wifi security )
To be honest I'm not sure if I'm gonna go this far in my abstract algebra class next time I teach it, but I'm considering my options
I was trying to get to the quintic and make the topics as accessible as possible, but I think it went over some of their heads :/
Because I thought the unsolvability of the quintic was a compelling enough focal point
you mean prove the unsolvability of the quintic?
Yeah
yeah especially cuz it's pretty easy to motivate and has a cool story
i agree
So much of the field theory links right back to stuff they've learned in high school
what about maybe t he trisecting problem
trisecting an angle iirc
or would that be boring
And answers fundamental questions like "how do we invent new numbers like i or √2"
Hmm, I didn't go into geometric constructibility
yeah
Ig the unsolvability of the quintic is the coolest motivator
in my "student" opinion haha
Yeah, but my students had a lot of trouble keeping definitions etc straight throughout the semester
Like a student told me they needed to look up what a field was every time they were asked about it
yeah i see
yeah ig it would be tough to like
introduce galois theory
more definitions regarding types of field extensions and so on
imo
Why not introduce covering theory
I think they were having trouble seeing the big picture
then ig ur thinking with like
this
I think this is the best way to go imo
Group applications 
u were talking about that right?
I just learnt that like some months ago
when learning aglebraic topology
and it's crazy
you can literally solve problems regarding free groups with just drawing some covering space of S^1 wedge S^1
it's so beautiful
For group applications, I was thinking of using the Rubik's cube as the grand motivator
yeah that's pretty cool too
or maybe chemistry too
spectroscopy ( things i dont know about :V )
I don't know much about the chemistry side of things other than like ... molecules have symmetries 🤷♂️
Is there quantum involved 
yeah definitely
omg what if
you
motivate symmetries a ton
then like
do the boring stuff ( the formal definitions, weird examples etc,..)
and then do cayley's theorem
boom
lmfao
as in like
every group is basically some subgroup of symmetry group
isn't that crazy
no, let the group act on the set of itself by multiplication 
Now the Cayley theorems on the other hand
yeahh
,rotate
ew
I am going to try to do all three of those
The first one I assume is like multiplying p_3 and p_2 and sieving out the extra repeating factors through power sums
symmetric polynomials are great
I assume I have to multiply p_2 * p_3 and sieve out terms I don’t want
Anything with a x_k^2 in it
How do i find a cyclic subgroup of order 8 in the group of units of Z32 without just guess and check
Im just calculating different things but seems inefficient
Do you what the group of units of Z/n looks like
Integers less than n relatively prime to n
What about the group structure?
I do not know
Sometimes cyclic sometimes not
I dont think ive learned theorems about group structure of that. Maybe i learn it later?
I have not learned the structure thm of finite abelin groups if thats what ur referring to
That comes later in my book
I think Arki just ask what is the composition law on (Z/n)^x
No
Composition law?
Then maybe they just expected you to trial and error
wdym by group structure then
It was just an application of some theorem about if G = HK and some other hypothesis, then G is direct product of H and K
Chinese remainder theorem to split it into a direct product
Then observing those rings, seeing if you can find a prime (which is cyclic of order one less than the prime)
Oh wait it’s 32
Z/2^5Z
It doesn’t even apply and I was about to assert that there’s a primitive root generator but it’s a power of 2 so that doesn’t even happen lmao
Oh ok
It’s the multiplicative group of elements coprime to 2 less than 32
I.e odd numbers between 0 and 32 (both exclusive)
Actually while I’m at it I might aswell try to find the structure of Z_2^k
(2n + 1)(2m + 1) = 4nm + 2(n + m) + 1
Let’s say we are in (Z_2^k)^x
(2^a + 1)(2^b + 1) = 2^(a + b) + (2^a + 2^b) + 1
Just immediately try finding the order of 3
@dull ginkgo you’re cracked
Thanks to this problem I realized that multiplicative groups mod n are fucked
You know, prime powers could be nice and all be cyclic y’know
But nah, powers of two have to be fucking “special”
fuck.
For the record $(Z/N)^* \cong \prod_{p|n} (Z/p^{n_p})^$ where $n_p$ is the largest power of p which divides N. Then $(Z/p^n)^ \cong (Z/p)^* \times Z/p^{n-1}$ when p is odd, and $Z/2 \times Z/2^{n-2}$ otherwise
Math_Discord_Final_Girl
I thought it’s cyclic
Wait no I am an idiot
except for 2 they are cyclic
but the powers of 2 ones are not
Unless n is small
Yeah the higher powers of 2 past 4 not being cyclic is stupid
I think it’s a product of cyclic of order 2 corresponding to <-1>
and <3> which has order 2^(n-1)
you think correctly
yep
Thanks to Kiand’s exercise ye
In general the additive part of Z/p^n * is generated by 1 + p
the rest is the elements from 1 to p-1, or their teichmuller lifts if you want to be fancy
Add it to my very few uses for CRT
- fully describing multiplicative groups mod b
- Artinian commutative rings are product of finitely many local rings assuming choice so the maximal exist lol
- Independence of characters over Fields (thus integral domains)
Idk what else it’s used for that don’t go down to those 3 cases though I did use it to make the world’s double indexing imaginable to torture my friend
They're not cyclic because the Carmichael function of 2^n is less than phi(2^n) for n>2, right? ie. no elements have order 2^n

I mean that’s kind of the byproduct I guess lmao
lambda(2^n) < phi(2^n) because Z/2^n is not cyclic? 
that’s the definition yes
I guess you could argue the implication goes both ways. But proving lambda(2^n) < phi(2^n) is relatively straightforward number theory, so that's the direction that makes most sense to me
was looking through my course outline, am i correct that the content coverage is on the low-end? It's a semester long course, 3 hour lectures/week for 13 weeks
This feels extremely like overcomplicated?
Let $s_k = \sum_{n = 1}^{N}{x_n^k}$. Now $f(x) = \prod_{n = 1}^{N}{(x - x_n)} = \sum_{n = 1}^{N}{(-1)^{N - n}p_{N - n}x^n}}$ \
Thus $f(x_n)x_n^m= 0$ for $1 \leq n \leq N$. So $0 = \sum_{n = 1}^{N}{f(x_n)} = \sum_{n = 1}^{N}{(-1)^{N - n}p_{N - n}s_{n+m}}$
THE TUBE
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Let $s_k = \sum_{n = 1}^{N}{x_n^k}$. Now $f(x) = \prod_{n = 1}^{N}{(x - x_n)} = \sum_{n = 1}^{N}{(-1)^{N - n}p_{N - n}x^n}}$ Thus $f(x_n)x_n^m= 0$ for $1 \leq n \leq N$. So $0 = \sum_{n = 1}^{N}{f(x_n)x_n^m} = \sum_{n = 1}^{N}{(-1)^{N - n}p_{N - n}s_{n+m}}$
slightly modified
THE TUBE
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either way does this like 10 second solution work lmao
I came up with that in like a fucking TENTH of the time it took to read the goddamn hint Jacobson gave which made 0 sense
I don't see a single goddamn issue with it
Let $s_k = \sum_{n = 1}^{N}{x_n^k}$. Now $f(x) = \prod_{n = 1}^{N}{(x - x_n)} = \sum_{n = 1}^{N}{(-1)^{N - n}p_{N - n}x^n}$ Thus $f(x_n)x_n^m= 0$ for $1 \leq n \leq N$. So $0 = \sum_{n = 1}^{N}{f(x_n)x_n^m} = \sum_{n = 1}^{N}{(-1)^{N - n}p_{N - n}s_{n+m}}$
chmowned
THE TUBE
YEAH
look at this guy tryna argue it rather than say it's obvious

waht a dummt
I'm so smart
tldr exchanging the summation signs
hi chuchu
What is meant by HOM(A,B) = B^A I think they mean cardinality of A and B
B^A is commonly used in set theory to denote the set of functions from A to B
Okay, thank you
i might just be blanking in this question but how do we extend the automorphism from F to F(u)
i think i'm not seeing the powers of u getting fixed when they are adjoined, because the rest of it falls into place just from the problem statement
A field automorphism of K is given
It is known that F and u are fixed
Show that this automorphism fixes F(u)
any element in $F(u)$ is a linear combination of powers of u with coefficients in $F$, since automorphisms are isomorphisms then we can break the polynomial into additions and multiplications that we know are fixed since coefficients are in $F$ which are already fixed, and powers of $u$ can be factored as $\sigma(u^n) = (\sigma(u))^n$?
HyacinthDroplet
Isn't the answer 6?
should be the lcm of the orders of each of the elements individually, can you show your work
$lcm(o(7),o(2),o(-k),o(-1))=lcm (6,1,2,2)=6$
Bilal ns
the order of 2 in Z_6 is 3 wrong as well
and -k in Q8
Sorry ,my mistake . it's number of elements of order 7 and 2 in $Z_{10}$ and $Z_6$
Bilal ns
? What was meant to be that number?
$lcm(o(7),o(2),o(-k),o(-1))=lcm (10,3,4,2)=60$
Bilal ns
Looks good 👍
is every separable extension galois
then why does galois closure exist
Given a separable extension K′ of K, a Galois closure L of K′ is a type of splitting field, and also a Galois extension of K containing K′ that is minimal, in an obvious sense.
no
to study general fields using Galois theory
huh
No, normal separable fields are Galois
normal?
what about abnormal ones?
Bizarre extensions…
A normal extension is an extension such that if one of the roots of a polynomial is in that extension, all of them are
I think. Correct me if I’m wrong
oh
ok thanks
also the minimal polynomial of any algebraic number is separable right
how would you prove this
or is this not right
isn’t this just the same definition as a splitting field
at least this should be true in Q right
all irreducible polynomials over a field of char 0 are separable
oh ok ty
No. A splitting field is for a specific polynomial. Here any polynomial with a root splits.
o ig smth like (x-a)^p=x^p-a^p isnt separable in char p field
A splitting field is a normal extension though
Generally a normal extension is a splitting field for a family of polynomials
ah i see okay
Though you can just multiply together all your polynomials right
In the finite case
The condition that any irreducible polynomial is seperable is called being perfect.
Any characteristic 0 field is perfect, like croq said. And also any finite field, or algebraic extension of Fp.
So for a field to be not perfect it would have to at least contain Fp(t) for some p.
Simplest example being
x^p - t
over Fp(t), which is irreducible but not seperable.
Poly is not separable iff it and its minimal poly share a root.
This proves any irreducible poly over char 0 field is separable.
Also makes clear that irreducible poly is not separable iff derivative is 0
this is a nice summary of it actually lol
like F_p(t) in some sense being universal for this
now is F_1 perfect
According to Wikipedia, field extensions of F1 are always given by 'adjoining roots of unity' and corresponds to cyclic groups. So I guess that should mean they're seperable...
So I guess that would make F1 perfect
I guess one should take some alggeo stuff that only works for perfect fields and check what happens
It’s perfect to me
It's perfect vacuously, as F_1 doesn't actually exist
Wait you mean you’re extending by cyclic groups or the extenstion IS a cyclic group?
The latter feels wrong to me
aren’t fields defined to have different additive and multiplicative identities
so how would F_1 be a thing
You don’t want to know
it’s not a literal field with one element
it’s a metaphor which is quite complicated and the correct object probably hasn’t been defined yet
It’s the thing you plug into, what I presume in generality are group schemes, to model what happens if you set q = 1 for formulas for things over F_q
there’s a sense in which number theory looks like algebraic geometry of “curves” over some “field” and the field with one element is supposed to be that “field”
This for instance turns GL(n, q) into S_n both globally and locally
Which is why I care
I feel like working with S_n is worse
what’s the typical progression after a galois theory course
That’s because you’ve never had to compute the reps of either of them.
Vector spaces over F_1 are supposed to be finite sets?
for many people it’s never using Galois theory again
Think about it like this. You’ve done group actions, which are F_1-reps. But you have not done vector space reps
I know what reps are. 8 reps is a set
i really liked the class i just had on it though
8? That’s cardio
Maybe for you
what would even be a field extension of F1
oh wait jagr mentioned it above, didn't read all
It should somehow be that there is a unique extension of size n for any n and all of them are the finite sets \mu_n
that’s my understanding
so that the maximal abelian extension of Q plays the role of \overline{F_p}(T)
Like Hom(F_(1^n), -) is the group scheme of nth roots of unity.
From what I've run into they're pointed sets. And F1-linear maps are maps of pointed sets that satisfy the first isomorphism theorem.
the only group of order 4 which is not cyclic
Does this definition make sense?
Yes
o thanks
Do you understand how I'd do part c here?
Do you understand this solution?
and it follows that because that, U_12 cannot be isomorphic to R_4.
Yes
But then how did they figure out U_12 is not isomorphic to V_4?
They perform the mod based calculations
and they similarly found out that there is no element of U_12 whose square is not the identity...
But why? Why is it isomorphic to V if there is no element of U_12 whose square is not the identity
wait
Good morning algebra
all elements can’t have an order of 2
just change it to all non-trivial
Sanity check time: The proof that a basis of a VS remains a basis under extension of scalars goes through for free modules right?
Yes, tensor products commute with direct sums (as well as all colimits)
Are you from Hawaii or something?
No just like to say good morning at odd times
Always morning somewhere I guess
What if he just goes to bed late?
Is morning relative to when you wake up, or relative to the day?
Is it always morning when one wakes up?
Good morning
The day I guess
Good meowning
Though I feel like people usually use it to mean strictly before 12pm
though actually like it seems more controversial as to when it begins
When it begins seems more relative to the person ig and I think that is just a social thing
unless you want to say it is after dawn or smth lol
Morning to me is the time between waking up and eating "lunch" whatever that means
So for me morning is about 20 minutes long
For me it's 5am-4pm 
How is 15:59 pm "morning"
Haven't eaten lunch yet, must be still morning
Hallo every-nyan
Do all adjunctions commute with colonists
Left adjoint commute with colomits
doesn't really make sense to say "adjunction" here, but rather "(in this case, left) adjoints"
And right adjoint commute with limits
this is formally dual (see there for more examples)
i can't tell if the misspellings here were intentional or not
(why are colonists commuting?)
Presumably the colony is quite far away, so they have to commute to their job. And I guess they all work as adjuncts at the university
Those left anyway.
The right adjuncts are those that limit commuting by moving to the city
You sometimes see them pair up in formal duels, fighting each other
I need to prove that Z[X] satisfies the divisor chain condition
Here’s my thoughts chat
Assume we have a strict chain of divisors where a_(n+1)(X) | a_n(X)
Obviously deg_(a_n+1) <= deg(a_n)
The degree of a nonzero polynomial has to always be positive (or zero) so by pigeonhole the degrees stabilize to some n
I am a stern believer of it is when you wake up.
And if a(X) | b(X) and deg(a) = deg(b), then a(X) * c = b(X) for some constant c in Z
I am trying to invoke contradiction here
Maybe think about a specific coefficients of a
If G is not abelian, does there have to exist a subgroup of G that is not normal?
If all subgroups of G are normal that does not imply G is abelian does it?
When the chain’s degrees stabilize, each successive term differs by an integer factor. The constant coefficient epimorphism fixes Z and thus the image of the chain after it stabilizes, which would give a strict chain of divisors in Z, a contradiction
Nontrivial subgroup I take you mean
yeah
Why is k being coprime with |H| needed? I thought I proved it but I didn't need to use that hypothesis
If G/H = <gH> then take K = <g> and it's easy to see G = KH and H intersection K is trivial argue by Lagrange's theorem the order of H ∩ K divides both k and |H| so it must be 1. Then take the internal semidirect product
Consider Q8 for example
what is Q8?
Quaternion group
Oh I have not looked at that example before
quaquaquaquaternions 
It has elements
{±1, ±i, ±j, ±k}
with i^2 = j^2 = k^2 = ijk = -1
You may want to double check why it's "easy to see"
Consider for example G = Z/4 and H = 2Z/4
It’s easy to see that every extension is split 
do you know the second smallest group with that property
https://planetmath.org/hamiltoniangroup
A group is Hamiltonian if and only if it is isomorphic to Q8×P for some torsion abelian group P that has no element of order 4.
So Q8 x C2 should be the next one
But in essence Q8 is kinda the only one
Q8 is also the smallest group with a representation with a nontrivial real (or for that matter, rational) Schur index!
Yeah that's right
The Schur index divides the degree, so in the first place it can only be the one of degree 2
you have to be 4 dim over the reals
Precisely!
because uhh something something Brauer group is C_2
Yes!
And guess what the endomorphism algebra of that real representation is?
is it H perchance
It may be H perchance
wow! almost like I didn't have too many choices!!
Ain't that cool?
I mean this is the simplest possible case, what else is it going to be
what is cool is that this lets you differentiate between D_8 and Q_8 character theoretically
with some information on centraliser sizes
Yeah!!!
Because otherwise Thifford Cleory makes their character tables the same aaaa
I love character theory
why are you using Thifford Cleory for such an assertion
bro forgot row orthogonality 😹
what is character theory about?
one ring isomorphism followed by combinatorics
i see
what is higher level combinatorics like?
I sucked at combinations and permutations problems so am i screwed
is it similar flavour?
i have not learned any combinatorics beyond very basics
basically, if you're given a representation and post-compose it with the trace map, this gives you a map G -> C, this map is the character of the represntation
these turn out to completely classify the representations up to isomorphism
that sounds cool
and they form a ring that's isomorphic to the ring of representations (including behaving very nicely with induction, restriction, and lifting)
with an inner product that tells you how representations decompose that you can compute incredibly easily
so instead of worrying about module theory you can just add little tuples together
that all sounds cool. Im excited to learn more algebra
They're both extensions of C_2 by C_4 with the same action 🗿
Trivial by clifford theory 
method of little groups............
nerd_emoji
wait
how are they the same action? D_8 splits, Q_8 doesn't
,w 2nd degree cohomology of C_4
The action of C_2 on C_4 is the same: inversion
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useless
yeah there's not really any other choice
I just don't like it
So the Clifford theory is the same (barring some questions about extension of characters) since the action only matters in the quotient
It's so sick
what the hell is a clifford...
The trace of a matrix is independent of the basis. So suppose you have a composition series for a finite-dimensional module of a k-algebra. Choose an appropriate basis, and you get block upper triangular matrices for every element of the algebra, and in particular taking the traces of these matrices will give you something depending only on the composition series.
In the rep theory of groups we look at the group algebra kG which is a k-algebra whose modules are representations of the group. If we have a module, we can take the trace of the action of each element of G. This gives us a function (typically not a homomorphism) chi : G → k, which is known as a character.
Fact: let k be a field of characteristic 0. Then two kG-modules are isomorphic if and only if their characters are equal.
Fact: Let k = C. There is a certain Hermitian inner product on 'class functions' which are functions G → k which are equal on conjugate elements. Then the set of characters of the simple modules form an orthonormal basis for the space of class functions.
These are two amazing results in elementary character theory.
I thought you were typing up a response to this. I am disappointed
A clifford is a big red dog
OK now for the clifford stuff
I can't neglect my poor wew
yeah just a slight elaboration would be nice
The two important results for me in clifford theory are a theorem in Isaacs which iirc isn't named, and Gallagher's theorem
So first
I know Gallaghers
that does sound epic. I dont know modules yet but im taking a course in them this fall
figured out the difference though, one is a central extenstion
Let $N \unlhd G$. Note that $G$ acts on $\operatorname{Irr}(N)$ by conjugation. Given $\chi \in \operatorname{Irr}(N)$, let $G_\chi = \build{g \in G}{{}^g\chi = \chi}$ -- Isaacs calls this the inertia group.
There is a bijection $\operatorname{Ind}{G\chi}^G \colon \operatorname{Irr}(G_\chi \mid \chi) \to \operatorname{Irr}(G \mid \chi)$.
sigh
Boytjie
inertia group is standard terminology
I kinda hate it ngl
and did you know that bijection holds block-wise?
I didn't! But I was aware that there is some nice Clifford theory of blocks
yurrr
I actually figured out the difference this time
I'm proud of u Wew
they're not extenstions of C_4. They're extenstions of C_2^2
D_8 is the split, Q_8 isn't
D_8 can be written as C_2 \wr C_2
Ah yes I see
or C_2^2 \ltimes C_2
So this is a twist you've done
swaggg





